CURIE TEMPERATURE - ELECTRICAL ENCYCLOPEDIA

CURIE TEMPERATURE

Curie Temperature — Definition, Formula & Applications

The Curie Temperature (also called Curie Point) is the critical temperature at which a ferromagnetic or ferrimagnetic material loses its permanent magnetic properties and becomes paramagnetic. Named after French physicist Pierre Curie (1859–1906), this phenomenon is fundamental to understanding magnetic material behaviour in electrical engineering, data storage, and industrial heating applications.

What is Curie Temperature?

Curie Temperature (Tc) is the temperature above which a magnetic material loses its spontaneous magnetisation and transitions from ferromagnetic (or ferrimagnetic) to paramagnetic behaviour. Below Tc, atomic magnetic moments are aligned in domains, producing strong net magnetisation. Above Tc, thermal energy overcomes the exchange interaction, randomising the moments.

  • Below Tc: Material is ferromagnetic — domains are aligned, strong magnetic response
  • At Tc: Phase transition occurs — spontaneous magnetisation drops to zero
  • Above Tc: Material becomes paramagnetic — weak, linear response to external field
Curie Temperature graph showing magnetisation vs temperature

The graph above shows how magnetisation decreases with rising temperature and drops sharply to zero at the Curie point.

Physics Behind the Curie Point

In ferromagnetic materials, neighbouring atomic magnetic moments are coupled by the quantum mechanical exchange interaction. This interaction favours parallel alignment of spins, creating magnetic domains. As temperature increases:

  • Thermal vibrations (lattice phonons) increase in amplitude
  • Individual atomic moments begin to fluctuate randomly
  • Domain walls become unstable and domain structure breaks down
  • At Tc, thermal energy (kBT) equals the exchange energy — long-range order is destroyed

This is a second-order phase transition — there is no latent heat, but the magnetic susceptibility diverges at Tc.

Curie-Weiss Law & Formula

Above the Curie temperature, the magnetic susceptibility of a material follows the Curie-Weiss Law:

χ = C / (T − Tc)

Where:

  • χ = magnetic susceptibility
  • C = Curie constant (material-specific)
  • T = absolute temperature (Kelvin)
  • Tc = Curie temperature (Kelvin)

The Curie constant is given by:

C = (N × μ₀ × μ²) / (3 × kB)

Where N is the number of magnetic atoms per unit volume, μ₀ is permeability of free space, μ is the magnetic moment per atom, and kB is Boltzmann's constant.

Curie Temperature of Common Materials

MaterialCurie Temperature (°C)Curie Temperature (K)
Iron (Fe)7701043
Cobalt (Co)11151388
Nickel (Ni)358631
Gadolinium (Gd)20293
Magnetite (Fe₃O₄)585858
Neodymium Magnet (Nd₂Fe₁₄B)310583
Alnico8601133
Permalloy (Ni₈₀Fe₂₀)596869
Curie temperature values for various materials

Effect on Different Magnetic Materials

The Curie temperature affects different classes of magnetic materials in distinct ways:

Material TypeBelow TcAbove TcExample
FerromagneticStrong magnetisation, aligned domainsParamagneticIron, Cobalt, Nickel
FerrimagneticUnequal antiparallel moments, net magnetisationParamagneticMagnetite, Ferrites
AntiferromagneticEqual antiparallel moments, zero net magnetisationParamagnetic (above Néel temperature)MnO, Cr₂O₃

Note: For antiferromagnetic materials, the transition temperature is called the Néel Temperature (TN), not the Curie temperature, though the physics is analogous.

Applications of Curie Temperature

Understanding Curie temperature is critical in several engineering domains:

  • Transformer Core Design: Silicon steel cores must operate well below Tc (770°C for iron) to maintain permeability. Overheating causes core saturation and increased losses.
  • Permanent Magnets: Neodymium magnets (Tc = 310°C) are unsuitable for high-temperature motors. Alnico or SmCo magnets are preferred for applications above 200°C.
  • Magnetic Data Storage: Hard disk drives use heat-assisted magnetic recording (HAMR) — a laser heats the medium near Tc to reduce coercivity during writing.
  • Induction Heating: Curie temperature limits the maximum temperature achievable by magnetic induction heating. Above Tc, the workpiece loses ferromagnetic coupling.
  • Fire Safety (Curie Point Thermometers): Magnetic fire alarms use a ferromagnetic element that releases a spring mechanism when heated above Tc.
  • Electric Vehicle Motors: PMSM motors in EVs must account for magnet demagnetisation risk if rotor temperature approaches Tc during sustained high-load operation.

Frequently Asked Questions

Q1: What happens to a magnet above Curie temperature?

Above the Curie temperature, a permanent magnet loses its magnetisation completely and becomes paramagnetic. The magnetic domains are destroyed by thermal energy. If cooled back below Tc without an external field, it will not regain its original magnetisation — it must be re-magnetised.

Q2: What is the Curie temperature of iron?

The Curie temperature of pure iron is 770°C (1043 K). Above this temperature, iron transitions from ferromagnetic to paramagnetic. This is why iron-core transformers must have adequate cooling to stay well below this limit.

Q3: What is the difference between Curie temperature and Néel temperature?

Curie temperature applies to ferromagnetic and ferrimagnetic materials (transition to paramagnetic state). Néel temperature applies to antiferromagnetic materials (transition to paramagnetic state). Both represent the temperature where long-range magnetic order is destroyed.

Q4: Can Curie temperature be changed by alloying?

Yes. Adding alloying elements changes Tc significantly. For example, adding chromium to iron lowers Tc, while adding cobalt raises it. Nd₂Fe₁₄B magnets have Tc raised by partial substitution of Dy or Tb for Nd.

Q5: Why is Curie temperature important in electrical engineering?

Curie temperature determines the operating temperature limit for magnetic components — transformer cores, motor magnets, relay contacts, and magnetic sensors. Exceeding Tc causes catastrophic loss of magnetic function, leading to equipment failure.